Controlled caustic generator surface lighting device forming a pattern on a target surface

ABSTRACT

The present invention relates to a vehicle turn indicator luminous device ( 1 ) comprising:
         an optical element ( 10 ) having a controlled caustic generator surface ( 12 ) so as to propagate a pattern over a usable range,   a mounting part ( 2 ) on which is intended to be mounted a beam generator ( 3 ) of rays incident on said generator surface,
 
the optical element being such that the propagated pattern is projected onto a target surface, visible from the exterior of the lighting device and situated in the usable range.

This application is a continuation-in-part of U.S. patent application Ser. No. 16/262,109, filed on Jan. 30, 2019, which is based upon and claims the benefit of priority from French Patent Application No. 18 50758, filed on Jan. 30, 2018 and French Application No. 1908799, filed on Jul. 31, 2019; the entire contents of which are incorporated herein by reference.

The present invention relates to the field of luminous devices emitting patterns onto a given surface, notably onto the road and more specifically to turn indicator luminous devices that indicate a change in the traveling direction of a vehicle or a turning direction of a vehicle at an intersection.

The document WO2016184721A1 discloses vehicle luminous devices comprising two transparent material plates the front and rear diopters of which each have a surface forming a matrix of optical lenses. A cache is disposed between the two plates. The cache and the optical lenses of each matrix are pressed together and are such as together to form a given light pattern on a target surface.

It is also known from document EP2543542 (also published under US2014328071) a vehicle with a turn signal lamp system, comprising a turn signal lamp which is installed in a head lamp housing of the vehicle, and comprises a first lamp unit configured to irradiate light forming a blinking pattern and a second lamp unit configured to irradiate light forming a road pattern to indicate the change in the traveling direction, wherein the second lamp unit includes a plurality of light source parts having a linear arrangement disposed adjacent to an exterior edge of the head lamp housing.

However, such known designs are complex and quite costly.

The technical problem that the invention aims to solve is therefore to simplify a vehicle turn indicator luminous device able to produce light patterns to project them onto a vehicle traveling surface, especially the road.

To solve this problem, the applicant has had the idea of using caustics.

Caustics are an optical phenomenon that have been known for a long time. They are for example observable at the bottom of a swimming pool lit by the sun. They form there fluctuating patterns forming overall a mesh of lines of more concentrated and therefore brighter light, with darker zones between the meshes. These lines and dark zones are caused by different fluctuations of the surface of the water. These fluctuations locally form variations of orientation with respect to the globally plane shape of the surface of the water. Accordingly, as a function of the local variations encountered, the rays are going to be deviated differently, some moving toward one another and forming the more concentrated and therefore brighter lines, and others moving away from each other and forming the dark zones. The meshing varies as a function of the agitation of the surface.

For a few years researchers have been interested in methods for using this phenomenon on fixed surfaces featuring local variations, to generate complex caustics of controlled shape. In particular, they have developed various methods for calculating refractive surfaces formed of a transparent material with a distribution and an arrangement of local variations such that, when these refractive surfaces are lit by a given light source, they enable a pattern to be formed on a screen.

In some of this work, this pattern, termed the target pattern, corresponds physically to a distorted image of the raised pattern that the local variations form, termed the subject pattern.

The applicant has realized that such surfaces could be used in vehicle turn indicator luminous devices.

The invention therefore relates to turn indicator luminous devices in which a controlled caustic generator surface deviates the light rays from a light source, this generator surface featuring local variations adapted to form a particular pattern on a given surface outside the vehicle, especially the vehicle traveling surface, usually the road.

To this end, a first object of the invention is a vehicle turn indicator luminous device comprising:

-   -   an optical element having a controlled caustic generator         surface, this generator surface being a reflecting or refracting         surface, extending in accordance with a given overall shape and         having local variations of shape about this given overall shape,         these local variations being distributed over the whole of said         generator surface so that they confer on the whole of the         generator surface a relief forming an object pattern, these         various local variations being such that the majority of said         generator surface is smooth and such that for a beam of rays         incident on the whole of said generator surface, these rays         having a given distribution, said generator surface deviates the         rays with different orientations as a function of the local         variations that they encounter, thus forming a deviated beam         propagating an identifiable propagated pattern over a usable         range extending in the upstream direction and at least as far as         a given finite optimum propagation distance, this propagated         pattern corresponding to a distorted projection of the object         pattern,     -   a mounting part on which is to be mounted a beam generator of         rays in accordance with the given distribution, so that the rays         are incident on said generator surface,         the optical element being such that the propagated pattern can         be projected onto a target surface, which is visible from         outside the luminous device and which is situated inside the         usable range and/or at a distance substantially equal to said         optimum distance.

By “identifiable” is meant that the pattern is recognized as that which will be observed at the optimum distance.

The best result is seen when the target surface is situated at a distance substantially equal to this optimum distance.

In the application, by “smooth” is meant a zone that can be differentiable at any point, in other words a zone free of projecting or recessed edges. A portion is smooth when all the points forming it conforms to this definition.

It is therefore possible to mount a light beam generator, such as a light source or a light source and a set of one or more optical elements, enabling generation of rays with a given distribution, so that these rays are incident on the optical element. Because of this, energizing the light beam generator will enable generation of the propagated pattern, which will propagate until it encounters a surface, in particular the target surface on which the vehicle travels.

The projection of the propagated pattern on the target surface forms the target pattern.

These beam generators can be simple. The optical element is sufficient in itself to modify the beam to make a pattern from it.

Moreover, this pattern is propagated over a finite given distance, namely over the usable range comprising the distance where the sharpness is the optimum, namely the optimum propagation distance, which allows some freedom in respect of the distance between the optical element and the target surface. The turn indicator luminous device according to the invention is simpler to assemble. This optimum propagation distance, referred to hereinafter as the optimum distance, is the distance at which the majority of the deviated rays forming the target pattern cross and therefore at which this pattern is sharpest. The generator surface can therefore be easily designed in relation to this definition.

Moreover, in contrast to the solutions with caches, in the luminous device in accordance with this first object, most, or even all, of the light rays encountering the generator surface are deviated and form the target pattern. The brightness of the target pattern is therefore greater with the turn indicator luminous device according to this first object.

The luminous device according to the invention may optionally comprise one or more of the following features:

-   -   the given distribution is substantially such that for any plane         transverse to, notably perpendicular to, the propagation         direction, at a given point of that plane, the ray or rays         incident at this point come from a single direction;     -   in the given distribution, the rays are substantially parallel         or substantially distributed in an emission cone;     -   the given distribution corresponds to that of a light-emitting         diode;     -   the luminous device comprises the ray beam generator in         accordance with the given distribution; the luminous device is         therefore ready to emit;     -   the generator surface comprises at least one smooth portion the         surface of which represents the majority of the generator         surface, the passage from one local variation to the other being         smooth inside this smooth portion;     -   the majority of the generator surface is such that each local         variation deviates the rays so as to form one and only one         portion of the target pattern that is distinct from the portions         of the target pattern formed by the other local variations and         for the majority of the target pattern each portion of the         target pattern receives light rays from one and only one local         variation; therefore, for this majority of the generator surface         and this majority of the target pattern, there is a bijective         relation between each smooth portion of the object pattern and         each portion of the target pattern with no marked brightness         discontinuity; this simplifies the calculation and therefore the         production of the generator surface.     -   all of the generator surface is smooth, the passage from one         local variation to the other being smooth; this moreover enables         less deformation of the image of the parts upstream of the         optical element; it is therefore possible either to see these         parts through the optical element, when the optical element is a         transparent element refracting the rays emitted by said beam         generator, or by observing the image of these parts on the         optical element, when the latter is a reflector reflecting the         rays emitted by said beam generator; this therefore enables         modification of the style of the beam generator;     -   the whole of the generator surface is such that each local         variation deviates the rays so as to form one and only one         portion of the target pattern that is distinct from the portions         of the target pattern formed by the other local variations and         for all the target pattern each portion of the target pattern         receives the light rays from one and only one local variation;         there is therefore a bijective relation between the whole of the         object pattern and each portion of the target pattern with no         marked brightness discontinuity; this simplifies the calculation         and therefore the production of the generator surface;     -   the passage between certain local variations is delimited by an         edge; a passage of this kind creates a discontinuity in the         slope variations over the generator surface; this makes it         possible to create very dark and even black zones and very         bright and narrow zones, such as clear writing;     -   the local variations are such that the rays of the deviated beam         do not cross short of said optimum distance; the target pattern         therefore remains sharp over a target surface positioned on the         upstream or at the optimum distance;     -   according to the preceding paragraph, there can also be a         minimum distance below which the pattern is not formed; in this         case, the pattern is sharp in a range, corresponding to the         usable range going from this minimum distance at least to the         optimum distance; for example, this range represents more than         half of the optimum distance;     -   the local variations have a tangent to the given overall shape         forming an angle between −60 and 60 degrees inclusive, notably         between −30 and 30 degrees inclusive; this enables good         transmission of the light rays;     -   each local variation has, at each of its points, an amplitude         defined as the distance between the local variation and said         overall shape along the normal and at a given point of the         overall shape;     -   the maximum amplitude of each local variation is in a range         between 0.001 millimetre and 1 millimetre inclusive; this         imparts a smoother appearance to the generator surface;     -   in an overall direction of propagation of the beam, the optical         element is circumscribed in a rectangle, one side of which         extending in a direction parallel to this propagation direction         is at least four times greater, notably six times greater than         that of the amplitude of each local variation relative to the         given local shape at the level of that local variation;     -   in an overall propagation direction of the beam, the generator         surface is circumscribed in a rectangle, one side of which         extending in a direction parallel to that propagation direction         is at least ten times greater, notably 30 times greater, than         that of one of the sides of a light source of the beam         generator;     -   the beam generator comprises a light source, notably a         light-emitting diode; light-emitting diodes are particularly         suitable for coupling to a controlled generator surface;     -   the beam generator comprises a light-emitting diode emitting its         rays generally in accordance with a cone; for example, the         generator may be formed only by one or more light-emitting         diodes;     -   the beam generator comprises a light source, notably a         light-emitting diode, and an optic adapted with the light source         to generate a beam of substantially parallel rays;     -   the optical element comprises a reflecting surface at least one         portion of which is formed by the generator surface; in other         words the generator surface is reflective; in particular, the         optical element may be a mask, notably metallized; in this case         the generator surface may form a portion of the surface of this         mask; another function may thus be conferred on the mask, such         as that of masking certain parts of the luminous device;     -   the optical element is made of a transparent material and is         arranged with the beam generator to form the beam diverted by         refraction of the rays emitted by the beam generator; this         allows a simple layout;     -   according to the preceding paragraph, the optical element         comprises an entry face for said rays arranged facing the beam         generator and an exit face for these rays arranged opposite said         entry face, the generator surface being formed on the entry face         or on the exit face;     -   in accordance with the preceding paragraph, the optical element         comprises two generator surfaces, a first generator surface         being formed on the entry face and a second generator surface         being formed on the exit face, these two generator surfaces         being arranged jointly to form the target pattern and to provide         the propagation over the optimum distance. This makes it         possible to allow greater freedom in the slopes to be conferred         on the local variations; moreover, this can also enable better         contrast to be obtained, or the depth field to be increased, or         even tend toward an infinite depth of field;

the luminous device comprises a housing and an outer lens closing the housing through which exit the light rays emitted by the luminous device, the closing outer lens forming the optical element, the generator surface being formed on the surface of a portion of the closing outer lens, the deviated beam being formed by refraction of the rays emitted by the beam generator; this therefore enables propagation of the target pattern outside the vehicle and without addition of any new part; for example, the luminous device may be such that once mounted on the vehicle the distance between the generator surface and the road in the direction of propagation of the target pattern corresponds to the usable range or is close to the optimum distance, according to a given orientation of the vehicle; this therefore enables projection of the light pattern onto the road; this distance between the closing outer lens and/or the generator surface may be equal to half the optimum distance, when the road is horizontal; in this latter case, this allows a visible sharp pattern whatever the orientation of the vehicle, climbing, descending, braking or accelerating.

The vehicle turn indicator luminous device according to the invention may be a dedicated (standalone) device, such as a turn signal lamp, or can for example be mounted (integrated) into:

-   -   a device for lighting the road, notably a front light or         headlamp, notably emitting a low beam and/or a long-range beam,         or a fog light;     -   a signalling device, notably a rear position light, a day         running light (DRL), a turn indicator, a stop light, a         high-level stop light, a rear fog light, a reversing light;

The invention also has for object a vehicle comprising a turn indicator luminous device according to the invention, notably connected to the electrical power supply of the vehicle.

The terms “upstream” and “downstream” refer to the direction of propagation of the light rays inside and outside the luminous device.

Unless otherwise indicated, the terms “front”, “rear”, “lower”, “upper”, “side”, “transverse” refer to the direction of emission of light from the corresponding turn indicator luminous device.

Other features and advantages of the invention will become apparent on reading the following detailed description of nonlimiting examples, for an understanding of which see the appended drawings, in which:

FIG. 1 is a diagrammatic view of a beam generator and an optical element of a luminous device according to a first embodiment of the invention;

FIG. 2 is an enlarged view of a portion of FIG. 1;

FIG. 3 is a diagrammatic view of a beam generator and an optical element of a luminous device according to a second embodiment of the invention;

FIG. 4 represents diagrammatically the propagation of a target pattern by a beam generator and an optical element of a luminous device according to the invention;

FIG. 5 represents diagrammatically a target pattern formed by a beam generator and an optical element of a luminous device according to the invention;

FIG. 6 represents diagrammatically the object pattern of the generator surface enabling generation of the target pattern from FIG. 5;

FIG. 7 represents a first example of a luminous device according to the invention;

FIG. 8 is a diagram of a second embodiment of the invention;

FIGS. 9a to 9f are diagrams of the various generator surface calculation steps.

FIGS. 1 and 2 illustrate an example of a turn indicator luminous device 1 according to the invention. These figures also make it possible to illustrate the general principle of the invention.

According to the invention, the turn indicator luminous device 1 comprises an optical element 10 having a controlled caustic generator surface 12. This generator surface 12 may a reflecting surface or a refracting surface, as shown in FIGS. 1 and 2. This optical element is referred to hereinafter as the caustic generator 10.

The generator surface 12 extends with a given overall shape 13 represented by the vertical dashed line in FIGS. 1 and 2.

More particularly, in the embodiment from FIG. 1, the caustic generator 10 is a transparent plate having an entry face 11 and an exit face. The entry face 11 is arranged facing a light ray beam generator 3 so as to receive the rays r₁, r₂, r₃ emitted by the beam generator 3. The exit face is arranged to receive the rays r₁, r₂, r₃ refracted by the entry face 11.

As in the example shown, the exit face may be formed, notably entirely, by the generator surface 12.

As a general rule, the generator surface 12 features local variations of shape around the given overall shape 13. These local variations are distributed over all of the generator surface 12 and so confer on the whole of the generator surface 12 a relief forming an object pattern.

For example, as shown in FIGS. 1 and 2, these local variations form recesses and bosses on the exit face of said caustic generator 10.

As a general rule, these various local variations are such that the majority of said generator surface 12 is smooth. For the majority of the generator surface 12, this surface is therefore differentiable at any point. In other words, over the smooth areas, it is free of projecting or recessed edges.

As a general rule, these various local variations are such that for the beam of rays r₁, r₂, r₃ incident on the whole of said generator surface 12, these rays r₁, r₂, r₃ having a known given distribution, the generator surface 12 deviates the rays r₁, r₂, r₃ with different orientations as a function of the local variations that they encounter, therefore forming a deviated beam propagating a light pattern over a usable range extending on the upstream side and at least as far as a given finite optimum propagation distance, termed the optimum distance, this propagated pattern corresponding to a distorted projection of the object pattern.

This generator surface 12 with its local variations corresponds to a controlled caustic generator surface.

Indeed, these local variations create local convergences and divergences of the rays. As these variations are local, a majority of rays move away from one another or toward one another without crossing before a certain distance. In the same way as the surface of a swimming pool through which sun rays pass creates a light pattern propagating and projecting onto the bottom of a swimming pool, the generator surface 12 creates a light pattern that propagates, the propagated pattern.

In the case of a swimming pool, this pattern generally propagates over a distance of 3 metres. The propagated pattern is therefore observable when projected onto the bottom of the swimming pool, whether the bottom is at 1.5 m or at 2 m. This bottom therefore forms the screen on which the caustic forming the propagated pattern can be observed.

In the case of a controlled caustic generator surface, like that of the invention, and depending on the local variations, the light pattern propagates at least over a given optimum distance. Beyond this optimum distance D_(p), the rays of the deviated beam cross.

In the context of the invention, and as can be seen in the FIG. 4 theoretical diagram, the optimum distance D_(p) is finite. If a screen is interposed at an intermediate distance D₁ or at another intermediate distance D₂, which are less than the optimum distance D_(p), the same pattern will be observed distorted to a greater or lesser degree.

Note that this optimum distance D_(p) is that at which the pattern will be sharpest. The generator surface can therefore be designed with reference to this definition.

There may equally exist a minimum distance D₀ below which the pattern is not formed. As a general rule this minimum distance D₀ is relatively short. This minimum distance D₀ may be a few centimetres, or even a few millimetres, depending on the application, such as an application to a motor vehicle luminous device. In this latter case it may be less than 1 centimetre (cm).

Equally, the pattern is not lost as soon as the rays cross but afterwards, at a greater maximum distance (not shown). It is however easier to design the generator surface relative to the crossing distance of the rays, which is defined more precisely than the distance at which it is considered that the pattern is lost. In the present application, this ray crossing distance is therefore termed the optimum propagation distance or optimum distance.

In other words, the usable range comprises a downstream portion, from the optimum distance D_(p) to this maximum distance, and an upstream portion, from the minimum distance D₀ to the optimum distance D_(p). The motif that can be observed at the optimum distance D_(p), if a screen is placed there, remains identifiable within these upstream and downstream portions.

In the case of the invention, this downstream portion may generally have a value different from that of the upstream portion. In particular, it may be less than more than half thereof.

For example, in a light with a sufficient closing outer lens portion, with an optimum distance D_(p) of 20 cm, a minimum distance D₀ of 1 cm, the value of the upstream portion would be 19 cm, and the downstream portion could be less than 9.5 cm.

In particular, said caustic generator 10 and its local variations are such that a propagated pattern is projected onto a target surface, which forms the screen, to form there a light pattern, termed the target pattern. This target surface is visible from outside the luminous device 1 and is situated at a distance within the usable range. The target surface may be at or near the optimum distance D_(p), which improves sharpness. The target surface is the surface on which the vehicle travels, notably a portion of the road.

As a general rule, to produce the generator surface 12, the latter is notably calculated taking into account the target pattern that it is wished to display, the shape of the target surface and its arrangement relative to the light rays forming the target pattern, together with the given distribution of the rays r₁, r₂, r₃ on emission by the beam generator 3, in particular their incidence on said caustic generator 10.

According to the invention, the given distribution may correspond to substantially parallel rays r₁, r₂, r₃ as shown in FIG. 3, or, notably, as shown in FIGS. 1 and 2, rays distributed substantially globally in an emission cone 14, notably with a divergent light source, such as an LED. This simplifies establishing the angle of incidence of the rays on said caustic generator 10, thus simplifying the calculation of the generator surface 12.

For this, it is possible to consider that the given distribution is such that for any plane perpendicular to the propagation direction, at any point of that plane, the ray or rays incident at that point come from a single direction. Indeed, the distribution of the rays emitted by an LED substantially corresponds to a given distribution of this kind.

To simplify the calculation, it is possible for the surface to comprise numerous discrete elementary surfaces and to compare the latter to the points mentioned in the preceding paragraph.

The turn indicator luminous device 1 may be shipped without the beam generator 3, but have a mounting part 2 on which it is intended to be mounted, so that the rays r₁, r₂, r₃ are incident on said generator surface 12.

In particular, this mounting part 2 and the beam generator 3 may be such that the beam emitted by the beam generator 3 when mounted has a given overall direction relative to said caustic generator 10. There is therefore no need at assembly time to adjust this orientation so that it corresponds to the arrangement enabling generation of the target pattern.

It is to be noted that these caustic generator surfaces do not necessitate great precision as regards the positioning of the beam generator 3. Assembly is therefore simplified.

In the example shown in FIG. 1, the beam generator 3 is mounted on the mounting part 2.

The beam generator 3 may as here be formed by a light-emitting diode (LED). In FIG. 1 there is diagrammatically represented a photo-emitting element 4 of the LED with, stuck on top, a transparent protective dome 5.

The target surface is a surface outside the vehicle, such as the road.

The methods of calculating this generator surface 12 may follow the following procedure, one example of which is shown in FIGS. 9a to 9 f:

-   -   in a step E1, termed the upstream step, shown in FIG. 9a ,         establish the relations defining the angle of incidence of the         rays r₁, r₂, r₃, r₄, r₅ and their distribution at each point of         the given overall shape 13, taking into account the given         distribution of the rays r₁, r₂, r₃, otherwise making it         possible also to define the brightness of each point at the         level of the given overall shape 13 on said caustic generator         10, termed the object point p₁, p₂, p₃, p₄, p₅,     -   in a step E2, termed the downstream step, which may be executed         before, after or at the same time as said upstream step E1,         define the luminous distribution over the target surface making         it possible to obtain the target pattern, and therefore define         the brightness at each point of the target surface 19, termed         the target point p′₁, p′₂, p′₃, p′₄,     -   then, in a correlation step E3, shown in FIG. 9b , establish a         relation between each object point p₁, p₂, p₃, p₄ p₅ and each         target point p′₁, p′₂, p′₃, p′₄, notably so that each target         point p′₁, p′₂, p′₃, p′₄ that receives light is associated with         only one or a set of object points p₁, p₂, p₃, p₄, p₅ making it         possible to obtain the brightness at these points required to         form the pattern,     -   thereafter, in a step E4/E5 of orientation of the local         variations, shown in FIGS. 9c to 9f , as a function of the         target points and object points associated by the relation         established in the correlation step E3, determine the         orientation of the local variations to be applied to the overall         shapes so that the rays r₁, r₂, r₃ r₄, r₅ incident at the object         points p₁, p₂, p₃, p₄, p₅ are deviated so as to have the         orientation enabling them to reach the target points p′₁, p′₂,         p′₃, p′₄ associated therewith via this relation.

The upstream step E1 takes into account the distribution of the rays upon their arrival at the level of the given overall shape 13. The simplest case, not shown, is that of an optical element 10, such as that shown in FIGS. 1 and 9 a, formed of a transparent plate the entry face 11 of which and the given overall shape 13 of the generator surface 12 are plane, and with a beam generator 3, such as that from FIG. 3, emitting parallel rays.

In this simple case, the beam generator 3 and said caustic generator 10 are such that the rays are perpendicular to the entry face 11. These rays are therefore not deviated before encountering the exit surface on which the generator surface is formed.

The embodiment from FIGS. 1 and 2 and FIGS. 9a to 9f represents an intermediate case in which the rays are distributed in an initial cone 14 at the outlet of the beam generator 3 and then refracted by the plane entry face, therefore remaining inscribed in a cone, enabling easy determination of the angle of incidence of the rays r₁, r₂, r₃, r₄, r₅ on the overall shape 13, and thus easy determination of the angle of incidence of the rays r₁, r₂, r₃, r₄, r₅ on the generator surface 12.

The embodiment from FIG. 3 represents another intermediate case in which the distribution of the rays r₁, r₂, r₃ is initially simpler, since they are parallel at the exit of the beam generator 3. On the other hand, they are then refracted differently by the entry face 11 because the latter is curved, for example a cylinder with a circular or elliptical section. However, this curvature being defined, it makes it possible to determine the orientation of the rays r₁, r₂, r₃ on their arrival at the level of the given overall shape 13 of the generator surface 12, which for its part is also curved.

In the example shown in FIG. 3, the optical element is a curved transparent plate, the entry face 11 of which and the general shape 13 of the generator surface 12 are cylindrical. So as to have parallel rays, the beam generator 3 may comprise a light source 6, such as a light-emitting diode, and a collimator lens 7 the diopters of which enable parallel orientation of the rays.

More complicated cases can however be envisaged, with

-   -   rays distributed in an emission cone,     -   a curved, notably cylindrical, entry surface, and     -   a generator surface of given curved overall shape.

It is equally possible to envisage other given distributions of the rays.

Concerning the downstream step E2, the simplest case is then for the target surface 19 to be plane and perpendicular to the overall direction of emission of the rays on arriving at the level of the overall shape 13 of the generator surface 12 to be calculated. The target pattern then corresponds to the propagated pattern.

In more complex cases, account must be taken of the orientation of the plane target surface, at an angle to the overall direction of transmission of the rays on arrival at the level of the generator surface. Such determination remains simple, however. It is more complicated, but achievable, when the target surface is not plane. Account must then be taken of its shape, notably to define it by an equation in order to determine the light distribution, so as to be able to observe the target pattern when projected. In all these more complex cases, the propagated pattern, if defined in a plane perpendicular to the propagation direction thereof, differs from the target pattern.

Thereafter, various methods may be used to carry out the step E3 of correlating the rays incident on the overall shape 13 of the generator surface 12 with the distribution of light over the target surface 19.

As explained above, this correlation step enables determination of which object points p₁, p₂, p₃, p₄, p₅ of the given overall shape 13 are associated with which target points p′₁, p′₂, p′₃, p′₄ of the target surface 19.

Thanks to the upstream step E1 the orientation of the rays r₁, r₂, r₃, r₄, r₅ on arrival at the level of the given overall shape 13 of the generator surface 12 is known. Moreover, the correlation between target points p′₁, p′₂, p′₃, p′₄ and object points p₁, p₂, p₃, p₄, p₅ determines the orientation of the rays r₁, r₂, r₃, r₄, r₅ on departing from this given overall shape 13 to join the object points p₁, p₂, p₃, p₄, p₅ to the target points p′₁, p′₂, p′₃, p′₄ with which they are correlated.

This therefore enables execution of the orientation step E4/E5, by calculating the variation to be assigned to the exit surface relative to this given overall shape 13 at all points of the latter, which enables definition of the generator surface 12.

Once this calculation has been done, it is therefore seen that, as a function of the amplitudes of the local variations, the generator surface 12 is at a greater or lesser distance from the given overall shape 13. To refine the calculation of the generator surface 12, it is therefore possible to repeat the upstream and downstream steps as well as the definition step, considering the arrival of the rays at their departure relative to the shape of the generator surface obtained previously and no longer relative to the given overall shape. The accuracy of this surface and therefore the sharpness of the image will improve with the number of iterations. Moreover, this also enables smoothing of the generator surface.

To carry out the orientation step, it is possible to use Descartes' laws, also known as Snell's laws in some English-speaking countries, or again as Snell-Descartes' laws.

Accordingly, in a substep E4, shown in FIGS. 9c and 9e , for an object point p₁, p₂, p₃, p₄, p₅ of the given overall shape 13 or of the generator surface calculated previously, with the direction of arrival and the direction of departure of the rays r₁, r₂, r₃, r₄, r₅, it is possible to determine the tangent {right arrow over (t)} and the normal {right arrow over (n)} of the exit surface at that point for which the latter deviates each incident ray r₁, r₂, r₃, r₄, r₅ arriving in the corresponding refraction direction.

In a substep E5, shown in FIGS. 9d and 9f , the generator surface 12 having these normals is determined by determining all of the normals {right arrow over (n)}, also known as normal fields.

FIGS. 9c and 9d illustrate the execution of these two substeps with magnification at the level of the object points p₁, p₂, p₃, not referenced in FIGS. 9c and 9d for greater clarity.

FIGS. 9e and 9f illustrate the execution of these two substeps with magnification at the level of the object points p₄, p₅ not referenced in FIGS. 9e and 9f for greater clarity.

In FIG. 2, there can be seen the local variations of the generator surface 12 relative to the given overall shape 13, which is plane in this example. These local variations correspond to changes of slope, defined by the normal {right arrow over (n)} and/or the tangent {right arrow over (t)} to the generator surface 12 at the level of the local variations. The result of this is that this generator surface 12 departs from the overall shape 13 and forms bosses and recesses.

For greater clarity the normals {right arrow over (n)} and tangents {right arrow over (t)} have been shown here for only three points on the generator surface 12, but the normal and/or the tangent is or are calculated for all the points.

The amplitude of a local variation may in this application be defined as the distance between the local variation and said overall shape 13 along the normal at a given point of the overall shape 13.

If the overall shape is plane, as in FIGS. 1 and 2, any point on the given overall shape can be defined by a dimension in a single direction z perpendicular to this overall shape 13.

There is seen in FIG. 2 a minimum amplitude a₁, by convention negative because it is situated on the upstream side of the generator surface 12, and a maximum amplitude a₂ downstream of the generator surface 12, by positive convention.

Note that in the method shown, it is possible to divide the surface into numerous discrete elementary surfaces and to compare the latter to the points p₁, p₂, p₃, p₄, p₅, p′₁, p′₂, p′₃, p′₄ referred to.

FIG. 5 illustrates the propagated pattern 16, as it will be seen on a flat screen perpendicular to the propagation direction and at a distance equal to or close to the propagation distance. If the target surface is also plane and oriented thus, then this propagated pattern 16 will also be the target pattern 16′ seen in FIG. 5. Otherwise, it will be deformed.

The generator surface 12 that made it possible to produce this propagated pattern 16 is shown in FIG. 6. Because of the relief formed on this surface 12, the object pattern 15 formed by this relief and therefore the local variations can be seen. This object pattern 15, symbolically represented in FIG. 6, corresponds to a distorted shape of the propagated pattern 16.

If the FIG. 5 pattern were also required to be the target pattern 16′ observed by a driver or a third-party observer observing the carriageway, the target pattern being formed by grazing incidence rays relative to the carriageway because coming for example from a headlamp, a rear light or a turn signal lamp, the propagated pattern would then have to be distorted relative to the target pattern, to observe the star on the road as represented in FIG. 5.

According to the invention, and as in FIGS. 1 and 2, the generator surface 12 may be such, and therefore calculated, so that, for the majority of the generator surface 12, namely smooth portions representing the majority of that surface, the passage from one local variation to the other is smooth. This is notably the case of the portion shown in FIG. 2. If for the calculations the local variations are not considered as points but as small zones of the generator surface, notably infinitesimally small zones, the generator surface 12 may moreover be such that, for these smooth portions, the local variations are smooth.

In particular, one of the smooth portions may have a surface representing the majority of the generator surface.

A first example calculation method may be used to calculate this generator surface 12. This is the method disclosed in the document Yue et al. [1]. That document notably indicates the various steps for constructing the generator surface 12 starting from a given example, in particular to establish the relation between the points of the generator surface 12 and those of the target surface.

This first method example enables a totally smooth generator surface 12 to be obtained. The passage from one local variation to the other is smooth.

To establish the relation of the correlation step, notably as in this first method, a condition is set as establishing a bijection between the object points and the target points. Accordingly, the whole of the generator surface 12 is such that:

-   -   each local variation deviates the incident light rays to form         one and only one portion of the target pattern 16′ that is         distinct from the portions of the target pattern formed by the         other local variations, and     -   for the whole of the target pattern, each portion of the target         pattern receives the light rays coming from one and only one         local variation.

This method enables good brightness gradients and good resolution. It may for example be used to produce the generator surface 12 from FIG. 1.

According to other methods, for improved contrast and to have darker zones and zones with maximum brightness, it is possible to adapt the local variations so that the generator surface 12 has one or more edges.

Depending on the case, the generator surface 12 comprises:

-   -   at least one edge delimiting portions of the generator surface         with different orientations so as to generate a divergence such         that certain zones of the target pattern receive virtually no         rays, or even no rays at all, thus forming dark zones, and/or     -   at least one edge delimiting portions of the generator surface         with different orientations so as to generate a convergence such         that certain zones of the target pattern receive the rays from a         plurality of local variations and/or a plurality of portions of         this generator surface.

This notably enables production of patterns with lines of light or very clear writing.

A second calculation method may be used for this, for example, to calculate the generator surface 12, as disclosed in the document Schwartzburg et al. [2].

In this second method, no bijection constraint is used in the correlation step. This method is more complex but enables a higher contrast to be obtained, namely a higher ratio between the light zones and the dark zones. This method in fact enables zones to be obtained darker than those of the Yue et al method mentioned above. With this second method it is therefore possible to obtain more marked demarcations between dark zones and light zones. The portions away from the edges are smooth, the passage from one local variation to the other being smooth.

In FIGS. 9a to 9f , for example, the method used does not impose a bijection constraint to establish the target pattern. At certain locations, a plurality of object points p₄, p₅ correspond to a single target point p′₄. The result of this is that the generator surface 12 features a slope variation discontinuity, corresponding to an outward edge 18 on the generator surface 12, and therefore inward in the direction of the incident rays. The local variations on either side of this edge 18 enable concentration of the rays r4, r5 on a line of the target surface, for example to form a sharp intense line.

Away from this edge 18, notably above and below it, the correlation step E3 has led, without constraining it, to a bijective relation between the corresponding object points p₁, p₂, p₃ and the corresponding target points p′₁, p′₂, p′₃.

Whatever the method used, each point on the generator surface 12 is therefore associated with an amplitude that corresponds to a distance from the overall shape 13, this amplitude being defined in a direction parallel to the normal to the overall shape 13 at that point.

As shown in FIGS. 1 and 3, for example, a plane is considered comprising the overall direction of the beam of incident rays. There is considered in this plane the rectangle 17 in which the caustic generator 10 is circumscribed, and this rectangle 17 may have a side length that is four times greater than, and notably six times greater than, that of the amplitude of each local variation relative to the given overall shape 13 at the level of that local variation, and therefore six times greater than the maximum amplitude.

Moreover, the local variations may have a tangent t forming an angle α with the given overall shape between −60 and 60 degrees inclusive, notably between −30 and 30 degrees inclusive.

Combining these slope and amplitude conditions yields optimum results, notably in terms of contrast and sharpness, notably enabling propagation of the propagated pattern over the usable range, in particular at the optimum distance D_(p).

It is to be noted that the smaller the light source 4, 6 of the beam generator 3 relative to the generator surface 12, the closer is the projected pattern to the required pattern used for the construction of the generator surface. For example, the side length of the rectangle 17 in which the caustic generator 10 is circumscribed may be at least ten times greater, notably thirty times greater, than that of a side length of that light source 3, 6, notably when that source is a light-emitting diode.

The two embodiments from FIGS. 1 to 3 are aimed at caustic generators 10 functioning by refraction.

Here the generator surface 12 is formed on an optical element 10 specifically dedicated to this. However, it may equally be formed on elements having other functions, such as a closing outer lens of the turn signal lamp or of the automotive lighting and/or signalling device into which the luminous device according to the invention is mounted, an optical lens, a mask.

In the application, “mask” denotes the embellisher intended to mask certain elements such as cables, the bottom of the housing. It is also known as a bezel.

Moreover, FIGS. 1 to 3 illustrate situations in which the generator surface 12 is on the exit face of the caustic generator 10. This is not limiting on the invention, however, and, generally speaking, the optical element can have a generator surface on the entry face and/or the exit face.

FIG. 8 illustrates a third embodiment in which the optical element 10′ or caustic generator 10′ functions by reflection.

Here the caustic generator 10′ is a mirror the reflecting surface of which forms the generator surface 12′, featuring local variations about its plane overall shape 13′.

This mirror 10′ may have one or more edges. Here, there is an inward edge 18′, namely forming the bottom of a recess, delimiting surface portions with an orientation facing one another, the latter portions therefore enabling creation of an intense line of light of particular shape on the target pattern, not shown.

The same construction methods may be applied to this reflecting generator surface 12′, taking into account during the various steps of the method that it is a question of reflection and not of refraction.

In such a case, the upstream step is simplified because the rays r₁, r₂, r₃, r₄ arrive directly on the generator surface 12 in accordance with the given distribution and also depart directly.

FIG. 7 shows a first example of luminous device according to the invention. In the case shown, a vehicle 20 with longitudinal axis X is equipped with two luminous devices according to the invention, which here are respectively integrated in a righthand rear light 21 and a lefthand rear light 22.

For example, each of these two rear lights 21, 22 includes a housing and a corresponding outer lens closing the housing. Each closing outer lens comprise a portion the diopter of which between the outer lens and the exterior forms the generator surface. Each of these generator surfaces receives some of the light rays coming from a light source of the corresponding rear light 21, 22. There could equally be provided a light source specifically dedicated to this generator surface.

The generator surface of the righthand rear light 21 is adapted to generate a target pattern 23 on the road forming a pattern made of a three triangles composition, here warning following vehicles of a change of direction to the right when considering the vehicle traveling direction illustrated by the X arrow.

FIG. 7 being an overhead view, this pattern is stretched out but will be perceived by following vehicles as less stretched. The object pattern, not shown, formed by the relief of the corresponding generator surface has a distorted form of this target pattern made of a three triangles composition.

In this example, it is clear that, in the propagation direction, the distance of the pattern between the generator surface and the target surface, namely the road, is going to vary as a function of the ride attitude of the vehicle 20, for example whether it is laden or not. Here the generator surface is such that when the ride attitude of the vehicle 20 is horizontal, on a horizontal road, the given optimum distance D_(p) is greater than, for example twice, the distance between the generator surface and the road in the direction of propagation of the propagated pattern. This makes it possible to have a visible sharp target pattern, whatever the orientation of the vehicle 20, in particular its ride attitude. The target pattern therefore remains visible when ascending, descending, braking or accelerating, and whatever the load.

In this example, the generator surface of the righthand rear light 21 receives the light rays from the light source enabling generation of a turn indicator signal.

It is to be noted that the lights could equally be constructed in accordance with the principle shown in FIGS. 1 and 3. In this case, instead of the generator surface being formed on the closing outer lens 9 closing the housing 8, the latter is, as described above, formed on a transparent plate 10 specifically designed to have the generator surface.

In the present invention, the target pattern is a logo, an icon (pictogram), a geometric figure, or an assembly of several logos, icons (pictogram), geometric figures or a combination thereof, such as an icon combined to one or several geometric figures. Advantageously, the geometric figure has a well recognisable shape, such as chevrons, triangles or disks. Advantageously, the icon shows a straight or bent (curved) arrow.

LIST OF REFERENCES

-   [1] Yonghao Yue, Kei Iwasaki, Bing-Yu Chen, Yoshinori Dobashi,     Tomoyuki Nishita. Poisson-Based Continuous Surface Generation for     Goal-Based Caustics, ACM Transactions on Graphics, Vol. 31, No. 3,     Article 31 (May 2014). -   [2] Yuliy Schwartzburg, Romain Testuz, Andrea Tagliasacchi, Mark     Pauly. High-contrast Computational Caustic Design, ACM Transactions     on Graphics (Proceedings of ACM SIGGRAPH 2014), Vol. 33, Issue 4,     Article No. 74 (July 2014) 

1. Vehicle turn indicator luminous device comprising: an optical element (10; 10′) having a controlled caustic generator surface (12; 12′), this generator surface being a reflecting or refracting surface, extending in accordance with a given overall shape (13; 13′) and having local variations of shape about this given overall shape, these local variations being distributed over the whole of said generator surface so that they confer on the whole of the generator surface a relief forming an object pattern (15), these various local variations being such that the majority of said generator surface is smooth and such that for a beam of rays (r₁, r₂, r₃) incident on the whole of said generator surface, these rays having a given distribution, said generator surface deviates the rays with different orientations as a function of the local variations that they encounter, thus forming a deviated beam propagating an identifiable propagated pattern (16) over a usable range extending in the upstream direction and at least as far as a given finite optimum propagation distance (D_(r)), this propagated pattern corresponding to a distorted shape of the object pattern, a mounting part (2) on which is to be mounted a beam generator (3) of rays in accordance with the given distribution, so that the rays are incident on said generator surface, the optical element being such that the propagated pattern is projected onto a target surface, which is visible from outside the luminous device and which is situated inside the usable range and/or at a distance (D₁, D₂) substantially equal to said optimum distance.
 2. Luminous device according to claim 1, in which the given distribution is substantially such that for any plane transverse to the propagation direction, at a given point of that plane, the ray or rays (r₁, r₂, r₃) incident at this point come from a single direction.
 3. Luminous device according to claim 1, in which the given distribution corresponds to that of a light-emitting diode.
 4. Luminous device according to claim 1, in which the luminous device comprises the beam generator (3) of rays (r₁, r₂, r₃) in accordance with the given distribution.
 5. Luminous device according to claim 1, in which the generator surface comprises at least one smooth portion the surface of which represents the majority of the generator surface (12; 12′), the passage from one local variation to the other being smooth inside this smooth portion.
 6. Luminous device according to claim 5, in which all of the generator surface (12) is smooth, the passage from one local variation to the other being smooth.
 7. Luminous device according to claim 6, in which the passage between certain local variations is formed by an edge (18, 18′).
 8. Luminous device according to claim 7, in which the beam generator (3) comprises a light-emitting diode (4,5).
 9. Luminous device according to claim 8, in which the beam generator (3) comprises a light source (6) and an optic (7) adapted with the light source to generate a beam of substantially parallel rays (r₁, r₂, r₃).
 10. Luminous device according to claim 9, in which the optical element (10′) comprises a reflecting surface at least one portion of which is formed by the generator surface (12′).
 11. Luminous device according to claim 10 in which the optical element (10′) is a mask.
 12. Luminous device according to claim 1, comprising a housing and an outer lens closing the housing through which exit the light rays emitted by the lighting device, the closing outer lens forming the optical element, the generator surface being formed on the surface of a portion of the closing outer lens, the deviated beam being formed by refraction of the rays emitted by the beam generator. 